Electrophoresis device

ABSTRACT

The invention aims to improve the spatial resolution in a multi-focus type electrophoresis apparatus that irradiates a capillary array from both ends thereof with laser beams. The invention relates to an electrophoresis apparatus in which capillaries at both ends of a capillary array are irradiated respectively with laser beams, and each of the two laser beams traverses multiple capillaries. In the electrophoresis apparatus, the laser beams are coaxially introduced into the capillary array from the both ends thereof to travel in a direction vertical to axis of each capillary and horizontal to the aligrnent plane of the capillary array; and a λ/4 plate and a polarizer are arranged on the laser beam optical axes. According to the invention, the total width of the incident laser beams is made narrow, generation of pseudo signals is prevented, and an analysis performance is improved.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a technology for separating and analyzing nucleic acids, proteins and the like by electrophoresis. The present invention relates to, for example, a capillary electrophoresis device.

2. Description of the Related Art

An electrophoresis method using a capillary has been used for such purposes as determination of DNA base sequences and base lengths. Multiple capillaries are required to be irradiated with exciting light in a capillary electrophoresis device, and methods for irradiating the multiple capillaries with light include a multi-focus method disclosed in Japanese Patent Application Publication No. 2001-324472.

In this method, samples each containing fluorescently-labeled DNA are introduced into the respective capillaries, and the capillaries are irradiated with a laser beam so that the laser beam can be transmitted through the multiple capillaries aligned in line. The capillary array is formed of the multiple capillaries aligned on a planar substrate, and a capillary in any one end or capillaries in both ends of a capillary array are irradiated with a laser beam. The laser beam is successively transmitted from one capillary to the next, thereby traversing the capillary array. The fluorescently-labeled DNA generates fluorescence by the laser beam with which the capillaries are irradiated. The luminescence generated from the capillary array is detected by a light detection device. By measuring the fluorescence generated by the capillaries one by one, DNA analyses on the samples introduced into the respective capillaries can be conducted. Analyses on proteins can be performed in the same manner.

In the multi-focus method, laser instability is caused by reflected and transmitted feedback light. Specifically, in a case where the capillary array is irradiated with a laser beam from only one end thereof, there is a problem that reflected light from a surface of the capillary array returns to a laser oscillator, and destabilizes laser oscillation thereof. On the other hand, in a case where the capillary array is irradiated with laser beams from both ends thereof, there is a problem that not only reflected light from the surfaces of the capillary array but also light having passed through the capillary array returns to a laser oscillator, and destabilizes laser oscillation thereof. In order to solve these problems, Japanese Patent Application Publication No. 2001-324472 shows a method in which angles are formed in the laser beams introduced into both ends of the capillary array.

SUMMARY OF THE INVENTION

The present inventors conducted studies to improve the analysis performance of the multi-focus method, and, as a result, found out the following problems.

As described in Japanese Patent Application Publication No. 2001-324472, in order to prevent from capillaries, laser beams may be introduced from both ends of a capillary array with its optical axis inclined at a certain angle, and be controlled to meet each other around the center of the capillary array where the laser beams from both the ends have almost the same irradiation intensity. In this case, however, the laser beams from both the ends do not meet each other in a vicinity of either of the ends of the capillary array. Consequently, the capillaries are irradiated with the laser beam thicker in appearance than each of the laser beams originally radiated.

Additionally, in a case where a laser beam is inclined to axes of the capillaries so as to prevent reflected feedback light, the incident laser beam is reflected in an interface between air and an external wall of each of the capillaries, and in an interface between gel and an internal wall of each of the capillaries. The reflected light beams are each also inclined to the axes of the capillaries, and thus is reflected multiple times, thereby generating multiple reflected light beams along axes different from an axis of the incident laser beam. As a result, the apparent diameter of the laser beam is large.

A laser beam with which the capillaries are irradiated is actually thick, and additionally, an intensity distribution of this laser beam is not expressed as an ideal Gaussian curve, but has a wide bottom. Thereby, a spectral shift is observed in measured data and a large pseudo signal is generated after matrix conversion of the data.

In a fragment analysis using a capillary electrophoresis device for the purposes of human identification and the like, reduction of this false signal is demanded. To meet this demand, the width of an incident laser beam on capillaries needs to be narrow. Incident laser beams from both end sides of the capillaries has the smallest diameter when these laser beams form one straight line, which is the ideal condition.

When orthogonal projections of the above two incident laser beams with respect to a plane formed by the capillary array are not substantially parallel to each other, the total diameter of these two laser beams joined together is larger than that of two laser beams coaxially emitted. Due to such large laser beam diameter, spatial resolution in fluorescence detection may be reduced. More specifically, in electrophoresis, DNA compositions are spatially separated in accordance with molecular weights while moving inside a capillary, and thus DNA bands are generated inside the capillary. In such electrophoresis, however, the large laser beam diameter may cause a reduction in resolution detection capability for these DNA bands.

In order to avoid such problem, it is desired that the centers of the two laser beams overlap each other in the vicinity of the center of the capillary array. By thus emitting the two laser beams, enlargement of the laser beam diameter can be suppressed to the minimum.

An object of the present invention is to improve spatial resolution in an electrophoresis device employing the multi-focus method in which a capillary array is irradiated with laser beams from both end sides thereof.

The present invention relates to a configuration of an electrophoresis device in which capillaries at both ends of a capillary array are irradiated respectively with laser beams, and each of the two laser beams traverses the plurality of capillaries. In the configuration: the laser beams are coaxially introduced into the capillary array from the both ends thereof to travel in a direction vertical to axis of each capillary but horizontal to the alignment plane of the capillary array; and a quarter wavelength plate and a polarizer are arranged on the laser beam optical axes.

According to the present invention, width of incident laser beams is made narrow, generation of false signal is prevented, and an analysis performance is improved.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a schematic diagram of an electrophoresis device according to one example.

FIGS. 2A and 2B are schematic diagrams of an optical system of a first embodiment of the present invention where a solid state laser source is used.

FIG. 3 is a schematic diagram of reflected feedback light and transmitted feedback light.

FIGS. 4A and 4B are schematic diagrams showing laser polarization directions according to a first embodiment of the present invention.

FIGS. 5A and 5B are schematic diagrams of an optical system of a second embodiment of the present invention where a solid state laser source is used.

FIG. 6 is a characteristic curve diagram of a beam splitter according to the second embodiment of the present invention.

FIGS. 7A and 7B are schematic diagrams of an optical system of a third embodiment of the present invention where a solid state laser source is used.

FIGS. 8A and 8B are schematic views of an optical system of a fourth embodiment of the present invention where a solid state laser source is used.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

Description will be given below of the above described and other innovative characteristics and advantages of the present invention in consideration of the drawings. However, the drawings are provided mainly for the explanatory purpose, and are not intended to limit the present invention.

In the following examples, disclosed is an electrophoresis device which is capable of blocking transmitted feedback light and reflected feedback light. In the electrophoresis device, a capillary array having a plurality of capillaries aligned in a plane is irradiated at both ends thereof respectively with laser beams; each of the laser beams is then transmitted through the capillaries from one to another so as to traverse the capillaries, thereby generating luminescence in each of the capillaries; and the luminescence thus generated is detected. In the electrophoresis device, the laser beams are coaxially introduced into the capillary array from the both ends thereof to travel in a direction vertical to the axis of each capillary and horizontal to the alignment plane of the capillary array, and a quarter wavelength plate and a polarizer are arranged on the axis of the laser beams so as to block transmitted feedback light and reflected feedback light.

Additionally, disclosed is an electrophoresis device a capillary array having a plurality of capillaries aligned in a plane is irradiated at both ends thereof respectively with laser beams; each of the laser beams is then transmitted through the capillaries from one to another so as to traverse the capillaries, thereby generating luminescence in each of the capillaries; and the luminescence thus generated is detected. In the electrophoresis device, the capillary array is irradiated from both ends thereof with two laser beams so that optical axes of the laser beams overlap each other, the quarter wavelength plate is arranged so that each of transmitted feedback light and reflected feedback light passes through the quarter wavelength plate twice, and the polarizer is arranged so as to be reached by the transmitted feedback light and reflected feedback light whose phases is rotated by 90 degrees through the quarter wavelength plate.

Additionally, disclosed is the electrophoresis device in which a solid state laser is used as a source of the laser beams.

Additionally, disclosed is the electrophoresis device in which a laser beam oscillated by a laser source is split into two laser beams by a beam splitter, the capillary array is irradiated with the two laser beams from both ends thereof, the polarizer is arranged in a route of the laser beam before the laser beam is split, and the quarter wavelength plate is arranged in each of routes of the laser beams after the laser beam is split.

Additionally, disclosed is the electrophoresis device in which, a laser beam oscillated by a laser source is split into two laser beams by a non-polarizing beam splitter (Non-polarizing half mirror), the capillary array is irradiated with the two laser beams from both ends thereof, and the polarizer and the quarter wavelength plate are arranged in a route of the laser beam before the laser beam is split.

Additionally, disclosed is the electrophoresis device in which, a laser beam oscillated by a laser source is split into two laser beams by a beam splitter, the capillary array is irradiated with the two laser beams from both ends thereof, and the polarizer and the quarter wavelength plate are arranged in each of routes of the laser beams after the laser beam is split.

Additionally, disclosed is the electrophoresis device in which, the laser beam is reflected by a mirror having a reflection characteristic in which phases of s-polarization light and p-polarization light are kept unchanged.

EXAMPLE 1

FIG. 1 is a schematic view of an electrophoresis device according to this example. A configuration of this apparatus will be described with reference to FIG. 1.

This apparatus is comprised of: a detection portion 116 used for optically detecting samples; a thermostatic chamber 118 used for maintaining capillaries at a constant temperature; a auto sampler 125 used for transporting various containers to the cathode end of the capillaries; a high-voltage power supply 104 used for applying a high voltage to the capillaries; a first ammeter 105 used for detecting a current generated by the high-voltage power supply; a second ammeter 112 used for detecting a current flowing in an anode electrode; a capillary array 117 formed by one or more capillaries 102; and a pump mechanism 103 used for injecting polymer into the capillaries.

The capillary array 117 is a replaceable member including 24 capillaries, and includes a load header 129, the detection portion 116, and a capillary head. When a measurement method is changed, the capillary array is replaced, and lengths of the capillaries are adjusted. Additionally, the capillary array 117 is replaced with a new one when there is damage to, or deterioration in quality of the capillaries.

Each of the capillaries is formed of a glass tube having an internal diameter of several ten to several hundred micrometers, and having an external diameter of several hundred micrometers. A surface of the capillary is coated with polyimide so as to be increased in strength. However, a light-irradiated portion of the capillaries to be irradiated with a laser beam is removed of the polyimide coating so that luminescence inside the capillary can easily come out. The inside of the capillary 102 is filled with a separation media so that imparted sample travels in different migration speeds during electrophoresis. While both fluid separation mediums and non-fluid separation media exist as separation mediums, a fluid polymer is used as the separation medium in this example.

The detection portion 116 is a member which acquires information depending on samples, and is irradiated with exciting light to emit light having wavelengths depending on samples. The vicinities of the light-irradiated portions of the 24 capillaries are fixedly arrayed on an optical flat plane with tolerances of several micrometers. During electrophoresis, the capillaries are irradiated from both ends thereof with two laser beams positioned substantially coaxially to each other, and the two laser beams successively pass through all of these light-irradiated portions. By these laser beams, information light (fluorescence having wavelengths depending on samples) is generated from the samples, and travels through the light-irradiated portions to the outside. This information light is detected by an optical detector 115, and the samples are analyzed.

Capillary cathode electrode 127 are fixed to the respective capillaries 102 through metallic hollow electrodes 126, whereby the capillaries have tips thereof protruding from the respective hollow electrodes 126 by about 0.5 mm. Additionally, all of the hollow electrodes 126 of capillaries are, as one body, mounted on the load header 129. Furthermore, all of the hollow electrodes 126 are electrically connected to the high-voltage power supply 104 installed in a main body of the apparatus, and thereby operate as cathode electrodes when it is necessary to apply a voltage, that is, when electrophoresis, sample introduction or the like is carried out.

Ends (the other end portions) of the capillaries, which are opposite to the capillary cathode electrode 127, are bundled together as one by the capillary head. The other end portions of the capillaries are members detachably attached in a pressure-resistant and air-tight condition in one bundle. The capillary head can be connected to a block 107 in a pressure-resistant and air-tight condition. Then, insides of the capillaries are filled with unused polymer by a syringe 106 from the other end portions. Replacement of polymer inside the capillaries is made every time measurement is newly conducted, so that performances of measurement can be enhanced.

The pump mechanism 103 is comprised of: the syringe 106; and a mechanism system used for pressuring the syringe 106. The block 107 is a connecting portion for causing the syringe 106, the capillary array 117, an anode buffer container 110, and a polymer container 109 to communicate with one another.

An optical detection portion is comprised of: a light source 114 used for illuminating the detection portion 116; and an optical detection device 115 used for detecting luminescence inside the detection portion 116. When the optical detection portion detects samples separated by electrophoresis in the capillaries, the light source 114 irradiates the light-irradiated portions of the capillaries, and the optical detection device 115 detects luminescence from the light-irradiated portions.

The thermostatic chamber 118 is covered with a heat insulating material and a heating/cooling mechanism 120 controls the temperature so that a temperature inside the thermostatic chamber 118 can be kept constant. Additionally, a fan 119 circulates and stirs air inside the thermostatic chamber 118, whereby temperatures of the capillary array 117 are kept uniform and constant regardless of positions thereof.

The auto sampler includes three electric motors and linear actuators, thereby being capable of moving in three axial directions, namely, vertical, horizontal, and depth directions. A moving stage 130 of the auto sampler 125 can carry at least one container thereon. The moving stage 130 is provided with an electrically-driven grip 131, by which a container can be held and released. Consequently, the auto sampler 125 can transport a buffer container 121, a washing container 122, a waste-liquid container 123, and a sample plate 124 being a sample container to the cathode electrode as necessary. Note that unnecessary containers are stored in a predetermined storage in the apparatus.

The apparatus main body 101 is used in a state connected to a control computer 128 via a communication cable. Through the control computer 128, an operator can control functions of the apparatus, and can receive data detected by the detection device in the apparatus.

FIGS. 2A and 2B are schematic views showing a detection portion of a capillary array, an optical detection portion, and introduction routes of laser beams in this example. A shutter and a filter are publicly known elements in this technical field, and are omitted for simplification. FIG. 2A is a side schematic view, and FIG. 2B is a front schematic view.

The optical detection portion in this example includes: a solid state laser 201 which oscillates a laser beam 202; a beam splitter 205 which splits the laser beam 202; reflecting mirrors 203 each of which changes a travelling direction of a laser beam; and laser condensing lenses 206 which condense laser beams toward the detection portion of the capillary array. Immediately after the solid-state laser 201, a polarizer 204 such as a sheet polarizer or a polarizing cube is arranged which is an optical element transmitting only light polarized in one direction. Additionally, two wavelength plates (quarter wavelength plate) 207 are arranged on both ends of the capillary array so that linear polarization of the laser beam 202 can be changed into circular polarization light before the laser beam 202 reaches capillaries 208. There, DNA is detected through observation of fluorescence emitted from the detection portion.

The detection portion of the capillary array is formed by having 24 capillaries 208 fixedly aligned on a reference base 209. Each of the capillaries is formed of a quartz glass tube coated with a polymer thin film. In the detection portion, polymer coating is removed and is set in a state where quartz is exposed. Internal and external diameters of the quartz glass tube are 50 μm and 320 μm, respectively, and an external diameter of each of the capillaries including the polymer thin films is 363 μm. A pitch between each adjacent ones of the capillaries is equal to the capillary external diameter, and is 363 μm, and a width of the capillary array is 8.7 mm obtained by multiplying 363 μm by 24. A plane formed by central axes of the 24 capillaries on the reference base 209, and a virtual plane obtained by extending the above plane to the whole space will be referred to as capillary-array aligned plane. Additionally, a virtual straight line existing on the capillary-array aligned plane, being vertical to the capillary axes of the 24 capillaries, and penetrating the center of the detection portion will be hereinafter referred to as an optical-axis base axis 210.

The laser beam 202 oscillated from the solid state laser 201, which is a light source of a laser beam, is changed in travelling direction by the reflecting mirror 203, passes through the polarizer 204, and is split into two beams by the beam splitter 205. The split laser beams are changed in travelling direction by the reflecting mirrors 203, and are introduced from both end sides of the detection portion of the capillary array.

Here, reflected and transmitted feedback light which are considered as a problem in this example will be schematically described by using FIG. 3. In this drawing, for the purpose of facilitating understanding of the reflected light and the transmitted light from the capillary array, incident light entering the capillary array is illustrated in a state slightly inclined with respect to a straight line vertical to the capillary axes.

When a laser beam enters the capillary array, reflection of the incident laser beam occurs in an interface between air and an external wall of each of the capillaries, and in an interface between gel and an internal wall of each of the capillaries. Particularly in the firstly mentioned air/external-wall interface, a refractive index is large, and an intensity of the reflected light is therefore high. Since there are two air/external-wall interfaces per capillary, reflection in the air/external-wall interfaces occurs 48 times in the capillary array formed of the 24 capillaries. If reflected feedback light 301 from this capillary array reaches the laser source, it destabilizes laser.

Additionally, transmitted feedback light 302 is transmitted light transmitted through the capillary array and emitted from an end side of the capillary array opposite from the side which the laser beam has entered. The transmitted feedback light 302 attenuates for amount equal to the reflected light, as compared to the incident light. If this transmitted feedback light 302 reaches the laser source, it destabilizes laser.

As a countermeasure against the feedback light, this example employs a configuration where, as show in FIG. 2, each laser beam 202 irradiates the detection portion of the capillary array after passing through the laser condensing lens 206 and the wavelength plate (quarter wavelength panel) 207. Here, the laser beam is condensed by the laser condensing lenses 206 (f=60 mm). Additionally, the wavelength plates (quarter wavelength panel) 207 change linear polarization of the laser beams 202 into circular polarization light. The laser beams 202 introduced from both ends of the detection portion of the capillary array is parallel to the capillary-array aligned plane, and is coaxial with respect to the optical-axis base axis 210.

A capillary which is located at one end of the capillary array and into which a laser beam is introduced will be hereinafter referred to as a first capillary. A distance between one of the laser condensing lenses 206 and the corresponding first capillary is 62 mm. The laser beam introduced into the first capillary is successively transmitted through one capillary to the next, and traverses the 24 capillaries.

A laser beam (transmitted feedback light) transmitted through the detection portion of the capillary array also passes through the wavelength plate (quarter wavelength panel) which is on the opposite side of the capillary array. That is, the laser beam 202 having been circularly polarized by one of the wavelength plates (quarter wavelength panel) is linearly polarized again by the other wavelength plate (quarter wavelength panel). At this time, a direction of this linear polarization is rotated 90-degrees from a direction of linear polarization of the laser beam 202 before being introduced into any one of the wavelength plates (quarter wavelength panel). The transmitted feedback light takes the same route as the incident laser beam, and reaches the polarizer 204 arranged immediately before the solid state laser 201. Here, the laser beam having passed through the wavelength plates (quarter wavelength panel) 207 twice is blocked by the polarizer 204, and the transmitted feedback light cannot reach the light source.

Additionally, as well as the transmitted feedback light, the reflected feedback light cannot reach the light source. Specifically, a laser beam (reflected feedback light) having been reflected by the detection portion of the capillary array again passes through the wavelength plate (quarter wavelength panel) which the laser beam has already passed through. That is, the laser beam 202 having been circularly polarized by the one of the wavelength plates (quarter wavelength panel) becomes linearly polarized again by the same wavelength plate (quarter wavelength panel). At this time, a direction of this linear polarization is rotated 90-degrees from a direction of linear polarization of the laser beam 202 before being introduced into any one of the wavelength plates (quarter wavelength panel). The reflected feedback light goes back a route which the laser beam 202 came, and reaches the polarizer 204 arranged immediately before the solid state laser 201. Here, the laser beam having passed through the wavelength plates (quarter wavelength panel) 207 twice is blocked by the polarizer 204, and the reflected feedback light cannot reach the light source.

Here, polarization of the feedback light will be described in detail by use of FIGS. 4A and 4B. The polarization of laser beam 202 before being introduced into the capillaries is linear polarization, and a direction of the polarization is a polarization direction 401. Linear polarization of the laser beam 202 is changed into circular polarization 403 by the wavelength plate (quarter wavelength panel) 207 provided before the capillaries 208, before the laser beam 202 reaches the capillaries 208. A crystal axis of each of the wavelength plates (quarter wavelength panel) 207 is rotated 45-degrees in respect to the polarization direction 401. The reflected feedback light 301 occurs from the laser beam 202 introduced into the capillaries 208. Polarization of the reflected feedback light 301 is circular polarization 403, and is changed back into linear polarization by passing through the wavelength plate (quarter wavelength panel) 207 again. At this time, a polarization direction of this linear polarization is a polarization direction 404. The polarization direction 404 is rotated 90-degrees from the polarization direction 401 which is the linear polarization of the laser beam 202 before being introduced into any one of the wavelength plates (quarter wavelength panel) 207.

Moreover, the polarization of transmitted feedback light 302 from the capillaries 208 is circular polarization 405, which is changed back into linear polarization through the wavelength plate (quarter wavelength panel) 207 on the other side of the capillaries 208 that the laser beam 202 have entered. At this time, a polarization direction of this linear polarization is changed into a polarization direction 406. The polarization direction 406 is rotated 90-degrees from the polarization direction 401 which is the linear polarization of the laser beam 202 before being introduced into any one of the wavelength plates (quarter wavelength panel) 207.

As has been described above, in this example, the reflected feedback light and the transmitted feedback light can be blocked through the countermeasure against the feedback light. Consequently, an electrophoresis device in which the laser beam 202 introduced from both ends of the capillary array is parallel to the capillary-array aligned plane, and are coaxial to the optical-axis base axis can be provided without causing instability in the laser source due to the feedback light. The laser beams are coaxially introduced into the capillary array from the both ends thereof to travel in a direction vertical to axis of each capillary but horizontal to the alignment plane of the capillary array. Thereby, width of the incident laser beams entering the capillaries is made narrow, generation of false signal is prevented, and an analysis performance is improved.

Additionally, a solid state laser is employed as the light source in this example. Since solid state lasers of some types are very unsusceptible to feedback light, configuration of the above laser beam optical axes is facilitated.

EXAMPLE 2

In this example, unlike Example 1, a wavelength plate (half wavelength plate) 207 is provided immediately after the polarizer 204. Example 2 will be described below while focusing on differences thereof from Example 1.

FIGS. 5A and 5B are schematic views showing a detection portion of a capillary array, an optical detection portion, and introduction routes of laser beams in this example.

In this example also, the laser beam 202 passes through the wavelength plate (half wavelength panel) 207 firstly, thereby becomes circular polarization light, and then, is introduced into the capillary array. Reflected feedback light and transmitted feedback light occurring as a result of the laser beam introduced into the capillary array pass through the wavelength plate (half wavelength panel) 207 again, is thereby changed back into linear polarization with its polarizing direction rotated 90-degrees from polarizing direction of the laser beam 202 first emitted, and then, is blocked by the polarizer 204.

However, it is necessary to prevent deformation of the circular polarization light by use of a non-polarizing beam splitter 501 at this time. A characteristic of the non-polarizing beam splitter 501 is shown in FIG. 6. In this characteristic, in a certain wavelength, both s-polarization light and p-polarization light show a reflectance of 50% and a transmittance of 50%, and phases of the lights are kept unchanged.

In this example, the number of the wavelength plates (quarter wavelength panel) 207 used in the apparatus can be set to one.

EXAMPLE 3

In this example, unlike Example 1, the laser condensing lenses 206 and wavelength plates (quarter wavelength panel) 207, which are provided on both ends of the capillary array in Example 1, are provided before reflection mirrors 701. Example 3 will be described below while focusing on differences thereof from Example 1.

FIGS. 7A and 7B are schematic views showing a detection portion of a capillary array, an optical detection portion, and introduction routes of laser beams in this example.

In designing the electrophoresis device, once a laser diameter and an f-value of each condensing lens, which are necessary for focusing the laser beam 202 toward the capillaries, are determined, a distance between the corresponding laser condensing lens 206 and the first capillary 208 cannot be shortened. As a result, spatial restriction in the apparatus designing arises.

In this example, the laser condensing lenses 206 and the wavelength plates (quarter wavelength panel) 207 are provided before reflecting mirrors 701. As a result, a spatial allowance is produced while the distance between the corresponding laser condensing lens 206 and the first capillary 208 is secured, whereby downsizing of the apparatus is achieved. Note that the reflection mirror 701 has a reflection characteristic in which phases of s-polarization light and p-polarization light are respectively kept unchanged.

EXAMPLE 4

In this example, further downsizing of Example 3 is achieved. Example 4 will be described below while focusing on differences thereof from Example 3.

FIGS. 8A and 8B are schematic views showing a detection portion of a capillary array, an optical detection portion, and introduction routes of laser beams in this example.

In this example, in order to provide a further downsized apparatus, the routes taken by the laser beam 202 in Example 3 are positioned to have angles which are not 90 degrees. While an angle between light incident to and reflected from the reflecting mirror 203 is set to 90 degrees by setting each of the incidence and reflection angles to 45 degrees in Example 3, the laser beam 202 can be positioned with arbitrary angles being formed therein in this example. Thereby, the laser beam 202 can be positioned without restriction, and further downsizing of the apparatus can be achieved. Note that deformation of the circular polarization light should be prevented by using a non-polarizing beam splitter 501. Additionally, the reflection mirrors 701 have a reflection characteristic in which phases of s-polarization light and p-polarization light are respectively kept unchanged.

While the examples of the present invention have been described hereinabove, the present invention is not limited to these examples, and those skilled in the art will understand that various alterations can be made thereto within the scope of the invention described in the scope of claims. Appropriate combinations of the respective examples are also included in the scope of the present invention.

DESCRIPTION OF REFERENCE NUMERALS

101 . . . apparatus main body, 102 and 208 . . . capillaries, 103 . . . pump mechanism, 104 . . . high-voltage power supply, 105 . . . first ammeter, 106 . . . syringe, 107 . . . block, 108 . . . check valve, 109 . . . polymer container, 110 . . . anode buffer container, 111 . . . electrode (GND), 112 . . . second ammeter, 113 . . . electrically-driven valve, 114 . . . light source, 115 . . . optical detection device, 116 . . . detection portion, 117 . . . capillary array, 118 . . . thermostatic chamber, 119 . . . fan, 120 . . . heating/cooling mechanism, 121 . . . buffer container, 122 . . . washing container, 123 . . . waste-liquid container, 124 . . . sample plate, 125 . . . auto sampler, 126 . . . hollow electrode, 127 . . . capillary cathode electrode, 128 . . . control computer, 129 . . . load header, 130 . . . moving stage, 131 . . . grip, 201 . . . solid-state laser, 202 . . . laser beam, 203 . . . reflecting mirror, 204 . . . polarizer, 205 . . . beam splitter, 206 . . . laser condensing lens, 207 . . . wavelength plate (quarter wavelength panel), 209 . . . reference base, 210 . . . optical-axis base axis, 301 . . . reflected feedback light, 302 . . . transmitted feedback light 

1. An electrophoresis device that detects luminescence generated from each of a plurality of capillaries, comprising: a capillary array having the plurality of capillaries aligned in a plane, being irradiated from both ends thereof respectively with laser beams and allowing each of the laser beams to be transmitted through the capillaries from one to another so as to traverse the capillaries, thereby generating the luminescence in each of the capillaries; a quarter wavelength plate; and a polarizer, wherein the laser beams are coaxially introduced into the capillary array from the both ends thereof to travel in a direction vertical to the axis of each of the capillaries and horizontal to the alignment plane of the capillary array, and the quarter wavelength plate and the polarizer are arranged on the axis of the laser beams so as to block transmitted feedback light and reflected feedback light.
 2. The electrophoresis device according to claim 1, further comprising a solid state laser as a source of the laser beams.
 3. The electrophoresis device according to claim 1, further comprising: a laser source oscillating a laser beam; and a beam splitter splitting the laser beam from the laser source into two laser beams, wherein the capillary array is irradiated from both ends thereof with the two laser beams, the polarizer is arranged in a route of the laser beam before the laser beam is split, and the quarter wavelength plate is arranged in each of routes of the laser beams after the laser beam is split.
 4. The electrophoresis device according to claim 1, further comprising a laser source oscillating a laser beam; and a non-polarizing beam splitter splitting the laser beam from the laser source into two laser beams, wherein the capillary array is irradiated from both ends thereof with the two laser beams, and the polarizer and the quarter wavelength plate are arranged in a route of the laser beam before the laser beam is split.
 5. The electrophoresis device according to claim 1, further comprising a laser source oscillating a laser beam; and a beam splitter splitting the laser beam from the laser source into two laser beams, wherein the capillary array is irradiated from both ends thereof with the two laser beams, and the polarizer and the quarter wavelength plate are arranged in each of routes of the laser beams after the laser beam is split.
 6. The electrophoresis device according to claim 5, further comprising a mirror having a reflection characteristic in which phases of s-polarization light and p-polarization light are kept unchanged, wherein the laser beam is reflected by the mirror.
 7. An electrophoresis device that detects luminescence generated from each of a plurality of capillaries, comprising: a capillary array having the plurality of capillaries aligned in a plane, being irradiated from both ends thereof respectively with laser beams and allowing each of the laser beams to be transmitted through the capillaries from one to another so as to traverse the capillaries, thereby generating the luminescence in each of the capillaries; a quarter wavelength plate; and a polarizer, wherein the capillary array is irradiated from both ends thereof with two laser beams so that optical axes of the laser beams overlap each other, the quarter wavelength plate is arranged so that each of transmitted feedback light and reflected feedback light passes through the quarter wavelength plate twice, and the polarizer is arranged so as to be reached by the transmitted feedback light and reflected feedback light whose phases is rotated by 90 degrees through the quarter wavelength plate.
 8. The electrophoresis device according to claim 7, further comprising a solid state laser as a source of the laser beams.
 9. The electrophoresis device according to claim 7, further comprising: a laser source oscillating the laser beam; and a beam splitter splitting laser beam from the laser source into two laser beams, wherein the capillary array is irradiated from both ends thereof with the two laser beams, the polarizer is arranged in a route of the laser beam before the laser beam is split, and the quarter wavelength plate is arranged in each of routes of the laser beams after the laser beam is split.
 10. The electrophoresis device according to claim 7, further comprising: a laser source oscillating the laser beam; and a non-polarizing beam splitter splitting the laser beam from the laser source into two laser beams, wherein the capillary array is irradiated from both ends thereof with the two laser beams, and the polarizer and the quarter wavelength plate are arranged in a route of the laser beam before being split.
 11. The electrophoresis device according to claim 7, further comprising a laser source oscillating the laser beam; and a beam splitter splitting the laser beam from the laser source into two laser beams, wherein the capillary array is irradiated from both ends thereof with the two laser beams, and the polarizer and the quarter wavelength plate are arranged in each of routes of the laser beams after the laser beam is split.
 12. The electrophoresis device according to claim 11, further comprising a mirror having a reflection characteristic in which phases of s-polarization light and p-polarization light are kept unchanged, wherein the laser beam is reflected by the mirror. 